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• W2962783013 endingPage "063403" @default.
• W2962783013 startingPage "063403" @default.
• W2962783013 abstract "In quantum mechanics, we define the measuring system $M$ in a selective measurement by two conditions. Firstly, when we define the measured system $S$ as the system in which the non-selective measurement part acts, $M$ is independent from the measured system $S$ as a quantum system in the sense that any time-dependent process in the total system $S+M$ is divisible into parts for $S$ and $M$. Secondly, when we can separate $S$ and $M$ from each other without changing the unitary equivalence class of the state of $S$ from that obtained by the partial trace of $M$, the eigenstate selection in the selective measurement cannot be realized. In order for such a system $M$ to exist, we show that in one selective measurement of an observable of a quantum system $S_0$ of particles in $S$, there exists a negative entropy transfer from $M$ to $S$ that can be directly transformed into an amount of Helmholtz free energy of $k_BT$ where $T$ is the thermodynamic temperature of the system $S$. Equivalently, an extra amount of work, $k_BT$, is required to be done by the system $M$." @default.
• W2962783013 created "2019-07-30" @default.
• W2962783013 creator A5041468878 @default.
• W2962783013 date "2018-06-08" @default.
• W2962783013 modified "2023-09-24" @default.
• W2962783013 title "Work required for selective quantum measurement" @default.
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• W2962783013 doi "https://doi.org/10.1088/1742-5468/aac13f" @default.
• W2962783013 hasPublicationYear "2018" @default.
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